1302.1860 (Ian A. Morrison)
Ian A. Morrison
We quantize linearized Einstein-Hilbert gravity on de Sitter backgrounds in a covariant gauge. We verify the existence of a maximally-symmetric (i.e. de Sitter-invariant) Hadamard state $\Omega$ for all globally hyperbolic de Sitter backgrounds in all spacetime dimensions $D \ge 4$ by constructing the state's 2-point function in closed form. This 2-pt function is explicitly maximally symmetric. We prove an analogue of the Reeh-Schlieder theorem for linearized gravity. Using these results we prove a cosmic no-hair theorem for linearized gravitons: for any state in the Hilbert space constructed from $\Omega$, the late-time behavior of local observable correlation functions reduces to those of $\Omega$ at an exponential rate with respect to proper time. We also provide the explicitly maximally-symmetric graviton 2-pt functions in a class of generalized de Donder gauges which are suitable for use in non-linear perturbation theory. Along the way we clarify a few technical aspects which led previous authors to conclude that these 2-pt functions do not exist.
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http://arxiv.org/abs/1302.1860
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